Let `v = K I^a T^b m^c ….(i)`
where K is dimensionless constant of
proportionality and a,b,c, are the dimensions of l, T
and m respectively to represent v.
The tension T stands for force whose
dimensions are `[M^1 L^1 T^(-2)]`
and `m = ("mass")/("length") =(M)/(L) = [M^1 L^(-1)]`
Writing the dimensions in (i), we get
`[M^0 L^0 T^(-1)] = L^a (M^1 L^1 T^(-2))^b (ML^(-1))^c`
`L^a M^b L^b T^(-2b) M^c L^(-c)`
`[M^0 L^0 T^(-1)] = M^(b+c) L^(a+b-c) T^(-2b)`
Applying the principle of hoomgeneity of
dimensions, we get
`b +c = 0 ...(ii)`
a +b - c = 0 ....(iii)
` -2b = -1 or b = (1)/(2)`
From (ii), `c = -b =-(1)/(2)`
from (iii), `a + (1)/(2) - (-(1)/(2)) = 0`
`a +(1)/(2) +(1)/(2) = 0 or a = -1`
Putting these values in (i), we get
`v = K I^(-1) T^(1//2) or v = (K)/(I) sqrt((T)/(m))`
Thisk is the required formula.